Method and apparatus for extracting parameters for an electrical structure

ABSTRACT

A parameter extraction technique for an electrical structure is based on a definition of network parameters that isolates pure mode responses of the electrical structure, and that makes mode conversion responses of the electrical structure negligible. A set of network parameters is obtained that represents pure mode responses for the electrical structure ( 410 ). These network parameters are processed to obtain model parameters that characterize each pure mode response ( 422, 424, 426, 428, 432, 434, 436, 438 ). Preferably, the mode specific parameters to combined to obtain mode independent parameters, such as coupling factor, propagation constant, and characteristic impedance values ( 440, 450 ).

This is continuation of application Ser. No. 08/939,117, filed Sep. 26, 1997, now U.S. Pat. No. 6,106,563 issued Aug. 22, 2000 and assigned to Motorola, Inc.

TECHNICAL FIELD

This invention relates in general to electrical circuit modeling, and more particularly, to parameter extraction techniques.

BACKGROUND

Behavioral model parameters are often used to understand the electrical and physical characteristics of components, circuits, and systems, required for a particular application. For example, the performance of a particular circuit component in a given circuit may be determined by employing model parameters to simulate that component. The prior art describes a number of approaches for obtaining parameters which vary in degrees of complexity, and effectiveness. A typical approach involves the use of network analyzers to measure the electrical response of a circuit, and to derive parameters based on this response. Substantial work has been done to characterize two-port devices in this manner.

Recently, there has been a significant increase in interest in characterizing differential and other multi-port devices. Of particular interest is the ability to understand the behavior of electrical structures having coupled signal lines. Multilayer ceramic couplers are examples of such structures. The prior art does not provide an adequate solution for quickly and accurately extracting parameters for these electrical structures. Therefore, a new approach for extracting behavioral model parameters is needed.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a block diagram of a first embodiment of a system for extracting parameters from an electrical structure, in accordance with the present invention.

FIG. 2 shows a block diagram of a second embodiment of a system for extracting parameters that uses a simulated electrical structure, in accordance with the present invention.

FIG. 3 is a summary of procedures used to obtain model parameters, in accordance with the present invention.

FIG. 4 is a summary of procedures used to derive model parameters from mixed-mode s-parameters, in accordance with the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

The present invention provides for parameter extraction for an electrical structure. This parameter extraction is based on a definition of network parameters in which mode conversion responses of the electrical structure are negligible, thereby allowing for isolation of the pure mode responses. In operation, a set of network parameters is obtained that represents pure mode responses for the electrical structure. These network parameters are processed to obtain model parameters that characterize each pure mode response. Model parameters refer to electrical design parameters, distributed parameters, physical parameters, and the like, that are used to characterize or model particular circuitry, or portion of circuitry, in an abstract manner. The parameter extraction technique described herein is particularly suitable for modeling linear networks.

In the preferred embodiment, the definition of network parameters corresponds to mixed-mode scattering parameters (s-parameters) that represent differential mode, common mode, and mode conversion responses for the electrical structure. The mixed-mode s-parameters are obtained such that the mode conversion responses are negligible. In one embodiment, the mixed-mode s-parameters are used to obtain electrical design parameters, such as a coupling coefficient, a characteristic impedance, and a propagation constant for each pure mode response. These mode specific electrical design parameters are then combined to provide corresponding mode independent parameters. In another embodiment, the mixed-mode s-parameters are processed to obtain mode specific distributed parameters. In yet another embodiment, the mixed-mode s-parameters are used to obtain physical dimensions for components of the electrical structure.

The definition of network parameters suitable for a given electrical structure is a significant aspect of the present invention. Preferably, the network parameters are defined to isolate the pure mode responses of the electrical structure, and to make negligible the mode conversion responses. In the preferred embodiment, the network parameters are s-parameters derived with respect to a reference base of a differential electrical structure having a transmission line comprising a coupled pair of signal lines. When the transmission line is stimulated by a differential signal, a differential mode voltage (V_(d)) exists as the difference between voltages V₁ and V₂ at a particular point, x, on the transmission line, where the subscripts (1, 2) represent corresponding points on the coupled pair of signal lines. Thus,

V(x)=V ₁ −V ₂.

A corresponding differential mode current (I_(d)) is defined as one-half (½) the difference between the respective currents I₁, I₂ traversing the coupled signal lines. Thus,

I _(d) (x)=½(I ₁ −I ₂).

A common mode voltage (V_(c)) on differential transmission line is defined with respect to the particular point as one-half (½) the sum of the respective voltages. Thus,

V _(c) (x)=½(V ₁ +V ₂).

The corresponding common mode current (I_(c)) is the total current flowing on both signal lines. Thus,

I _(c)(x)=I ₁ +I ₂.

The characteristic impedance of each mode (Z_(d), Z_(c)) can be defined as a ratio of the forward propagating wave component (V_(d) ⁺, V_(c) ⁺) of the voltage (V_(d), V_(c)) to the forward propagating wave component (I_(d) ⁺, I_(c) ⁺) of the current (I_(d), I_(c)) of the appropriate modes at any point, x, along the transmission line. Thus,

Z _(d) =V _(d) ⁺(x)/I _(d) ⁺(x);

Z _(c) =V _(c) ⁺(x)/I _(c) ⁺(x);

These values can be used to derive normalized wave equations.

Imposing the condition of low-loss transmission lines on the coupled pair, the characteristic impedances are approximately purely real. Under this condition, Z_(d)≈R_(d), and Z_(c)≈R_(c), where R_(d) and R_(c) are the real portions of Z_(d) and Z_(c), respectively. For a differential electrical structure having first and second ports, the normalized wave equations at the first port (x=0) can be stated as: $a_{d_{1}} = {{\frac{1}{2\sqrt{R_{d}}}\left\lbrack {{V_{d}(x)} + {{I_{d}(x)}R_{d}}} \right\rbrack}{_{x = 0}{b_{d_{2}} = {{\frac{1}{2\sqrt{R_{d}}}\left\lbrack {{V_{d}(x)} - {{I_{d}(x)}R_{d}}} \right\rbrack}{_{x = 0}{a_{c_{1}} = {{\frac{1}{2\sqrt{R_{c}}}\left\lbrack {{V_{c}(x)} + {{I_{c}(x)}R_{c}}} \right\rbrack}{_{x = 0}{b_{c_{2}} = {{\frac{1}{2\sqrt{R_{c}}}\left\lbrack {{V_{c}(x)} - {{I_{c}(x)}R_{c}}} \right\rbrack}{_{x = 0}.}}}}}}}}}}}$

A similar derivation can be made for the second port.

Mixed-mode scattering parameters can be represented by a matrix [S], such that:

[b]=[S][a];

where [a] and [b] denote n-dimensional column vectors, and [S] denotes an n-by-n matrix. The generalized mixed-mode two-port s-parameters can be stated as: $\begin{bmatrix} b_{d_{1}} \\ b_{d_{2}} \\ b_{c_{1}} \\ b_{c_{2}} \end{bmatrix} = {\left\lbrack \frac{S_{dd}S_{dc}}{S_{cd}S_{cc}} \right\rbrack \begin{bmatrix} a_{d_{1}} \\ a_{d_{2}} \\ a_{c_{1}} \\ a_{c_{2}} \end{bmatrix}}$

where [S_(dd)] is a 2-by-2 matrix of s-parameters representing the pure differential mode response of the electrical structure, [S_(cc)] is a 2-by-2 matrix of s-parameters representing the pure common mode response of the electrical structure, [S_(dc)] and [S_(cd)], are matrices of s-parameters representing mode conversion or cross-mode responses of the electrical structure. In particular, [S_(dc)] describes the conversion of common mode waves into differential mode waves, and [S_(cd)] describes the conversion of differential mode waves into common mode waves. For substantially differential circuits, the mode conversion matrices [S_(dc)], [S_(cd)] ordinarily contains zeroes or negligible values.

The derivation of mixed-mode s-parameters for differential structures is described in U.S. Pat. No. 5,495,173, issued to Bockelman et al. on Feb. 27, 1996, for a Method And Apparatus Characterizing A Differential Circuit, the entire contents of which are hereby incorporated by reference. Similar derivations can be made to obtain network parameters that isolate pure mode responses of other types of electrical structures.

For an ideal differential circuit, a set of mixed-mode s-parameters (S_(MIX)) represents a definition of network parameters having negligible or zero mode conversion values. These mixed-mode s-parameters may be generated by a mathematical transformation of well known standard s-parameters (S_(STD)), as follows:

S _(MIX) =MS _(STD) M ^(*T);

where M is a matrix defined as: ${M = {1/{\sqrt{2}\begin{bmatrix} 1 & {- 1} & 0 & 0 \\ 0 & 0 & 1 & {- 1} \\ 1 & 1 & 0 & 0 \\ 0 & 0 & 1 & 1 \end{bmatrix}}}};$

and (^(*T)) represents a transpose and complex conjugate of the matrix M.

The above concept can be extended to define network parameters S_(X) having negligible or zero mode conversion values for an arbitrary four-port circuit by an appropriate transformation matrix M_(x) applied to standard four-port s-parameters S_(STD). The relevant values can be developed as follows:

Let, ${M_{x} = \left\lbrack \quad \begin{matrix} a_{11} & a_{12} & a_{13} & a_{14} \\ a_{21} & a_{22} & a_{23} & a_{24} \\ a_{31} & a_{32} & a_{33} & a_{34} \\ a_{41} & a_{42} & a_{43} & a_{44} \end{matrix}\quad \right\rbrack};$

where α_(ij) represent complex numbers.

Let,

S _(X) =M _(X) S _(STD) M _(X) ^(*T).

Partition S_(X) such that all partitions are two-by-two (2×2) matrices. Thus, ${S_{X} = \left\lbrack \frac{S_{11}S_{12}}{S_{21}S_{22}} \right\rbrack};$

where S₁₁, S₁₂, S₂₁, and S₂₂ are two-by-two (2×2) matrices. Modes are then defined by finding α_(ij) such that:

[S ₁₂]=[0]and [S ₂₁]=[0].

This operation forces mode conversion values to be zeroes. The values for the matrix M_(X) can then be derived using the above equation and appropriate values for S_(STD) determined through measurement, simulation, or the like. The rows of M_(X) define the new modes in terms of single ended waves.

FIG. 1 shows a block diagram of a first embodiment 100 of a system for extracting parameters from an electrical structure, in accordance with the present invention. A measurement system 120 has equipment coupled to a device under test (DUT) 110 to provide a data source 101. The data source 101 is coupled to a computer processing system 105 that includes a memory 130, a parameter extraction processor 140, and a data output module 150. In the preferred embodiment, the DUT 110 is an electrical structure comprising coupled transmission lines. The measurement equipment is capable of developing mixed-mode s-parameters from data generated from the DUT 110. In operation, the measurement equipment 120 stimulates the DUT 110 using differential and common mode input signals 125. The DUT 110 provides corresponding differential and common mode output signals 115 to the measurement equipment 120. The measurement equipment 120 provides mixed-mode s-parameters 127 which are stored in the memory 130. Thus, in the preferred embodiment, the mixed-mode measurement system 120 operates to stimulate the particular electrical structure 110 and to generate therefrom a set of mixed-mode scattering parameters that comprises distinct sets of network description parameters.

FIG. 2 shows a block diagram of a second embodiment 200 of a system for extracting parameters that uses a simulated electrical structure, in accordance with the present invention. Here, a device simulator 220 is coupled to a device model 210 to provide a data source 201. The device simulator 220 uses the device model 210, which provides data 215 characterizing a particular electrical structure, to simulate characteristic responses of the modeled electrical structure. The device model 210 may represent a physical model of the electrical structure. Preferably, the device simulator 220 operates to provide these characteristic responses in accordance with a definition of network parameters that isolate pure mode responses. In the preferred embodiment, the simulator models the particular electrical structure and generates therefrom a set of mixed-mode scattering parameters that comprises distinct sets of network description parameters. As in FIG. 1, the data source 201 provides network parameters 127 to the memory 130 of the computer processing system 105.

Referring to FIG. 1 and FIG. 2, the memory 130 contains distinct sets of network description parameters that characterize pure mode responses of the electrical structure 110, or the structure represented by the device model 210. In the preferred embodiment, the distinct sets of network parameters correspond to the [S_(dd)] and [S_(cc)] matrices described above, which represent the pure differential mode response, and the pure common mode response of a differential circuit. The parameter extraction processor 140 is coupled to the memory 130 and has an input 135 of the distinct sets of network description parameters. The processor is responsive to the input 135 to process each distinct set of network description parameters to obtain mode specific model parameters, and to generate mode independent model parameters based on a combination of the respective mode specific model parameters. The model parameters generated from the parameter extraction processor 140 are coupled to the data output module 150 for display or for further processing.

FIG. 3 is a summary of procedures 300 used to obtain model parameters, in accordance with the present invention. Sets of network parameters are obtained which represent pure mode responses of an electrical structure, based on a definition of network parameters in which mode conversion responses of electrical structure are negligible, step 310. These network parameters may be derived from direct measurements taken from a stimulated electrical structure, or from data generated by a simulator configured using an appropriate device model. Each set of network parameters is processed to obtain model parameters that characterize pure mode response, step 320.

FIG. 4 is a summary of procedures 400 used to derive model parameters of coupled transmission lines from mixed-mode s-parameters, in accordance with the present invention. Network parameters are obtained which represent an electrical structure, step 410. In the preferred embodiment, the network parameters are mixed-mode s-parameters, and the electrical structure comprises coupled transmission or signal lines having a differential mode response and a common mode response. According to one embodiment, the mixed-mode s-parameters are generated from direct measurement of differential and common mode output waves of a differentially stimulated circuit. According to another embodiment, the mixed-mode s-parameters are generated from a mathematical transformation of multi-port s-parameters derived for a particular circuit, such as described above. According to yet another embodiment, the mixed-mode s-parameters are generated from a simulated circuit. The mixed-mode s-parameters are processed to obtain mode specific parameters, included propagation constant and characteristic impedance values for differential mode and common mode based signal propagation.

For common mode specific parameters, a set of common mode s-parameters is selected from the mixed-mode s-parameters, step 422. The s-parameters representing the common mode response are converted into a matrix of ABCD parameters, step 424. The ABCD parameters can be represented in matrix form as: $\left\lbrack \quad \begin{matrix} A_{c} & B_{c} \\ C_{c} & D_{c} \end{matrix}\quad \right\rbrack;$

where A_(c), B_(c), C_(c), and D_(c) represent common mode parameter values. The value A_(c) is used to determine a product of propagation constant and length (γ_(c)L), step 426, where:

γ_(c) L=cos h−1(A_(c)).

The value B_(c) and the product γ_(c)L are used to determine a characteristic impedance (Z_(c)), step 428, where:

Z _(c) =B _(c)/sin h(γ_(c)L).

Similarly, for differential mode specific parameters, a set of differential mode s-parameters is selected from the mixed-mode s-parameters, step 432. The s-parameters representing the differential mode response are converted into a matrix of ABCD parameters, step 434. The ABCD parameters can be represented in matrix form as: $\left\lbrack \quad \begin{matrix} A_{d} & B_{d} \\ C_{d} & D_{d} \end{matrix}\quad \right\rbrack;$

where A_(d), B_(d), C_(d), and D_(d) represent differential mode parameter values. The value A_(d) is used to determine a product of propagation constant and length (γ_(d)L), step 436, where:

γ_(d) L=cos h−1(A _(d)).

The value B_(c) and the product γ_(d)L are to used determine a characteristic impedance (Z_(d)), step 438, where:

Z _(d) =B _(d)/sin h(γ_(d) L).

Alternatively, network parameters such as t-parameters may be used with reformulated equations to derive similar values.

The model parameters specific to each mode response are combined to obtain mode independent electrical design parameters. Thus, the mode specific characteristic impedances Z_(c), Z_(d) are used to determine a mode independent characteristic impedance, Z_(oo), step 440, where:

Z _(oo) ={square root over (Z_(d)Z_(c))}.

These values, Z_(c), Z_(d), and Z_(oo), are used to determine a mode independent coupling coefficient, c, step 450, where: $c = {\frac{1 - \left( \frac{Z_{d}}{Z_{oo}} \right)^{2}}{1 + \left( \frac{Z_{d}}{Z_{oo}} \right)^{2}}.}$

According to the present invention, the mixed-mode s-parameters are used to derive other model parameters. Particularly, mode specific distributed parameters are determined, including resistance per unit length (R_(c), R_(d)), inductance per unit length (L_(c), L_(d)), capacitance per unit length (C_(c), C_(d)), and conductance per unit length (G_(c), G_(d)) for a physical electrical model, based at least in part on the coupling coefficient, propagation constant, and characteristic impedance. These parameters can be derived using the following relationships: ${Z_{d} = \sqrt{\frac{R_{d} + {j\quad \omega \quad L_{d}}}{G_{d} + {j\quad \omega \quad C_{d}}}}};$ ${\gamma_{d} = \sqrt{\left( {R_{d} + {j\quad \omega \quad L_{d}}} \right)\left( {G_{d} + {j\quad w\quad C_{d}}} \right)}};$ ${Z_{c} = \sqrt{\frac{R_{c} + {j\quad \omega \quad L_{c}}}{G_{c} + {j\quad \omega \quad C_{c}}}}};$ $\gamma_{c} = {\sqrt{\left( {R_{c} + {j\quad \omega \quad L_{c}}} \right)\left( {G_{c} + {j\quad w\quad C_{c}}} \right)}.}$

The mixed-mode s-parameters are also used to obtain physical model parameters. In particular, the mixed-mode s-parameters are used to determine physical dimensions for components of the electrical structure based at least in part on the mode specific distributed parameters and the electrical design parameters. A closed form function of mixed-mode parameters is developed in terms of the physical design elements. In one embodiment, field simulation software such as method of moments is used to solve for an array of physical implementations of the structure being considered. The array is over the set of physical parameters that are to be determined. For example, the physical parameters of a symmetrical broadside coupled stripline structure would be the conductor width (w), spacing between the coupled conductors (s), and the spacing between the ground planes enclosing the coupled conductors (b). Once the array of mixed-mode values are solved for the structure, a polynomial function is fitted to the measurements with the parameters w, s, and b in the polynomial relation. Subsequent mixed-mode measurements could then be used with these developed polynomial based relations to determine the physical values of the measured structure.

The present invention provides for significant benefits that facilitate the design of differential and other electrical structures. Model parameters extracted using the described techniques provide for more accurate and complete analysis of electrical designs. These model parameters can be derived for particular component, circuit, and system designs, and made available in libraries for use in the design of more complex circuits and systems. 

What is claimed is:
 1. A method of extracting design parameters for an electrical structure, comprising the steps of: generating sets of network parameters representing pure mode responses from measurements derived from the electrical structure, wherein a pure mode response is such that mode conversion responses of the electrical structure are negligible; and processing each set of network parameters to obtain model parameters that characterize each pure mode response, wherein the model parameters represent physical and/or electrical design characteristics of the electrical structure, and wherein the model parameters comprise a coupling coefficient, a characteristic impedance, and a propagation constant for each pure mode response of the electrical structure.
 2. The method of claim 1, wherein the step of obtaining comprises the step of generating the sets of network parameters from direct measurement of differential and common mode output waves of the electrical structure stimulated in a differential mode and a common mode.
 3. The method of claim 1, wherein the electrical structure comprises coupled transmission lines having a differential mode response and a common mode response.
 4. The method of claim 3, wherein the step of extracting comprises: converting a subset of the sets of network parameters representing the differential mode response into a first matrix of ABCD parameters, $\left\lbrack \quad \begin{matrix} A_{d} & B_{d} \\ C_{d} & D_{d} \end{matrix}\quad \right\rbrack;$

determining a product of propagation constant and length (γ_(d)L) where: γ_(d) L=cos h ⁻¹(A _(d)); and determining a characteristic impedance (Z_(d)), where: Z _(d) =B _(d)/sin h(γ_(d) L).
 5. The method of claim 4, wherein the step of extracting comprises: converting a subset of the sets of network parameters representing the common ode response into a second matrix of ABCD parameters, $\left\lbrack \quad \begin{matrix} A_{c} & B_{c} \\ C_{c} & D_{c} \end{matrix}\quad \right\rbrack;$

determining a product propagation constant and length (γ_(c)L) where: γ_(c) L=cos h ⁻¹(A _(c)); and determining a characteristic impedance (Z_(c)), where: Z _(c) =B _(c)/sin h(γ_(c) L).
 6. The method of claim 5, further comprising the steps of combining model parameters specific to each pure mode response to obtain mode independent electrical design parameters, including the steps of: determining a mode independent characteristic impedance, Z_(oo), where: Z _(oo) ={square root over (Z_(d)Z_(c))}; and determining a mode independent coupling coefficient, c, where: $c = {\frac{1 - \left( \frac{Z_{d}}{Z_{oo}} \right)^{2}}{1 + \left( \frac{Z_{d}}{Z_{oo}} \right)^{2}}.}$


7. The method of claim 1, further comprising the steps of combining model parameters specific to each pure mode response to obtain mode independent electrical design parameters.
 8. The method of claim 7, wherein the model parameters comprise a coupling coefficient, a characteristic impedance, and a propagation constant for each pure mode response of the electrical structure.
 9. The method of claim 8, wherein the step of processing further comprises the step of determining mode specific distributed parameters including a resistance per unit length (R), an inductance per unit length (L), a capacitance per unit length (C), and a conductance per unit length (G) for a physical electrical model, based at least in part on the coupling coefficient, propagation constant, and characteristic impedance.
 10. The method of claim 9, further comprising the step determining physical dimensions for components of the electrical structure based at least in part on the mode specific distributed parameters and the model parameters.
 11. A system for extracting parameters to model a particular electrical structure, comprising: a memory that contains distinct sets of network description parameters that characterize pure mode responses of the particular electrical structure, wherein a pure mode response is such that mode conversion responses of the electrical structure are negligible; and a processor coupled to the memory and having an input of the distinct sets of network description parameters, the processor being responsive to the input to process each distinct set of network description parameters to obtain mode specific model parameters, and to generate mode independent model parameters based on a combination of the respective mode specific model parameters, wherein the mode independent model parameters represent physical and/or electrical design parameters for the electrical structure, and comprise at least two of a coupling coefficient, a characteristic impedance, and a propagation constant.
 12. The system of claim 11, further comprising a mixed-mode measurement system coupled to the particular electrical structure and to the memory, wherein the mixed-mode measurement system operates to stimulate the particular electrical structure and to generate therefrom a set of mixed-mode scattering parameters that comprises the distinct sets of network description parameters.
 13. The system of claim 11, further comprising a simulator coupled to the memory, wherein the simulator models the particular electrical structure and generates therefrom a set of mixed-mode scattering parameters that comprises the distinct sets of network description parameters. 